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RESEARCH PAPER
The April 24, 2013 Changning Ms4.8 earthquake: a feltearthquake that occurred in Paleozoic sediment
Xiangfang Zeng • Libo Han • Yaolin Shi
Received: 27 September 2013 / Accepted: 2 January 2014 / Published online: 22 January 2014
� The Seismological Society of China, Institute of Geophysics, China Earthquake Administration and Springer-Verlag Berlin Heidelberg 2014
Abstract The dense broadband seismic network provides
more high-quality waveform that is helpful to improve
constraint focal depth of shallow earthquake. Many shal-
low earthquakes occurring in sediment were regarded as
induced events. In Sichuan basin, gas industry and salt
mining are dependent on fluid injection technique that
triggers microseismicity. We adopted waveform inversion
method with regional records to obtain focal mechanism of
an Ms4.8 earthquake at Changning. The result suggested
that the Changning earthquake occurred at a ESE thrust
fault, and its focal depth was about 3 km. The depth phases
including teleseismic pP phase and regional sPL phase
shows that the focal depth is about 2 km. The strong, short-
period surface wave suggests that this event is a very
shallow earthquake. The amplitude ratio between Rayleigh
wave and direct S wave was also used to estimate the
source depth of the mainshock. The focal depth (2–4 km) is
far less than the depth of the sedimentary layer thickness
(6–8 km) in epicentral region. It is close to the depth of
fluid injection of salt mining, which may imply that this
event was triggered by the industrial activity.
Keywords Induced earthquake � Depth phase �Waveform inversion
1 Introduction
An earthquake sequence including the Ms4.8 mainshock
(Changning earthquake for short) shocked Changning,
Sichuan, on April 25, 2013, which injured dozens and
resulted in economic losses amounting to about 300 million
RMB (Fig. 1). The Chinese Earthquake Network Center
reported that both the Ms4.8 mainshock and the strongest
aftershock occurred at a depth of 4 km. (http://www.cenc.
ac.cn/manage/html/402881891275f6df011275f971990001/
__SUBAO/_content/13_04/25/13e3e2158b900.html), while
the USGS National Earthquake Information Center deter-
minated the mainshock is a M5.3 event occurring at 10-km
depth (http://comcat.cr.usgs.gov/earthquakes/eventpage/usb000
gfau#summary). Such divergence increases more interest in
improving accuracy of focal parameters.
Most deconstructive and felt earthquakes in Sichuan
occur at major fault systems such as the Longmenshan
Fault system. However, the epicenter of Changning earth-
quake is about 40 km away from the Huayingshan Fault
that is a major fault in eastern Sichuan basin. Since the
thickness of sediment in southern Sichuan depression
ranges from 6 to 8 km (Song and Luo 1995), the Chang-
ning earthquake was eventually an earthquake occurring in
sediment. Because the strength of rock in shallow crust is
too weak to accumulate enough strain, most earthquakes
occur in the middle crust except in the area with anomaly
geothermal flow (Shi and Zhu 2003; Klose and Seeber
2007). Therefore, there are only a few articles about
deconstructive earthquakes occurring in shallow crust
(\5 km) in India and Austria cratons (Dawson et al. 2008;
Gupta et al. 1996). Luo et al. (2011) reported a decon-
structive event occurring in Mesozoic sediment at the
center of Sichuan basin. The 2010 Christchurch earthquake
is also another recent example (Kaiser et al. 2012). Such
X. Zeng � Y. Shi (&)
CAS Key Laboratory of Computational Geodynamics,
University of Chinese Academy of Sciences, Beijing 100049,
China
e-mail: [email protected]
L. Han
Institute of Geophysics, China Earthquake Administration,
Beijing 100081, China
123
Earthq Sci (2014) 27(1):107–115
DOI 10.1007/s11589-014-0062-3
cases provide an opportunity to study strain accumulation
and failure in weak rock.
In recent years, production of shale gas experienced a
great boom in the US, and many countries proposed
ambitious plans for shale gas exploration and production.
Because the permeability of shale or other tight rocks is
very low, engineers pump huge volumes of pressurized mix
of water, chemicals, and sand to create and hold open
fractures. Seismicity events induced by fluid injection in
geothermal sites (e.g., Eberhart-Phillips and Oppenheimer
1984) and wastewater disposal sites (e.g., Healy et al.
1968) have been reported in the recent decades. Several
moderate and felt earthquakes (up to Mw5.7, Keranen et al.
2013) occurred in shale-gas fields in the US midcontinent,
and such a situation was proposed to be posing a higher
risk (Ellsworth 2013). There are several articles on induced
seismicity in gas field (Zhu et al. 2007; Long et al. 2010)
and salt mine (Lu et al. 2009). Changning–Weiyuan field is
the first shale-gas production area of China. The historical
seismicity concentrates in the range of 10–20-km depth.
Therefore, the Changning earthquake is a rare case study to
analyze seismic hazard caused by shallow event.
Due to sparsity of the sample, uncertainties of source
parameters of shallow earthquake determinated with
104˚36' 104˚48' 105˚00' 105˚12'
28˚00'
28˚12'
28˚24'
28˚36'
28˚48'
10 km 0 10 20 30
20130424_Ms4.8
200608012006092220070814 20071005
Fig. 1 Historical seismicity (M [ 2.0) between 2009 and 2013 at Changning. The red star denotes location of salt mine
108 Earthq Sci (2014) 27(1):107–115
123
traditional methods are sizable. For travel-time location
except nearby stations, sparse samples of takeoff vector in
upper hemisphere increase uncertainty introduced by
tradeoff between depth and origin time (Mori 1991). For
first motion inversion, uncertainties of the depth and
velocity model also introduce large errors. Methods based
on waveform could use more information taken from later
phases to constrain fault plane and centroid depth. In this
article, we adopted waveform inversion method to obtain
focal mechanism including centroid depth, and then used
local and teleseismic depth phases and amplitude ratio of
body wave and surface wave to determinate the focal
depth.
2 Focal mechanism
The cut and paste (CAP for short) method is a popular
waveform inversion method, which uses regional three-
component records of body wave and surface wave to
constrain fault plane and centroid depth (Zhao and Helm-
berger 1994; Zhu and Helmberger 1996). Recently, the
teleseismic waveform was also introduced into CAP to
provide more constraint for thrust event (Ni et al. 2010;
Chen et al. 2012). We collected three-component records at
stations within 200 km (Fig. 2a; Zheng et al. 2009) and
adopted Sichuan basin velocity model obtained from short-
period surface-wave dispersion inversion (Fig. 2b; Xie
et al. 2012). Velocity increases with the depth in sediment,
and the total thickness of the crust reaches 40 km. Syn-
thetic seismograms of arbitrary faults are built from those
of the three basic faults that were computed with FK
method (Zhu and Rivera 2002). Both synthetic and
observed waveforms were bandpass filtered (0.02–0.15 Hz
for body wave and 0.02–0.1 Hz for surface wave). Grid
search scheme was employed to seek the best solutions at
different depths, and the misfit function reaches the mini-
mum at 3 km as the best centroid depth (3 km; Fig. 3a),
while the magnitude of moment is 4.5. The fault planes of
the best solution are 128�/42�/83� (plane I) and 317�/48�/96� (plane II) for strike, dip, and rake, respectively. Fig-
ure 3b shows comparison between the filtered synthetic
and observed waveforms. Most cross-correlation coeffi-
cients of Pnl Segment are larger than 0.8 except CQT and
WAS stations that are further away from the epicenter. For
surface-wave segment, the synthetic waveforms best fit
observations at ROC and YAJ stations, and the cross-cor-
relation coefficients are larger than 0.7. Strike of fault plane
I is consistent with the Changning Anticline, and it is close
to fault planes of historical events obtained from the
amplitude ratio method (Ruan et al. 2008). Consequently,
the fault plane I is possibly the rupture plane.
(a) (b)
Fig. 2 a Epicenteral and seismic stations used in this study. Star denotes epicenter, while triangles show stations. Faults are shown in solid lines,
b basin velocity model. Dashed line denotes shear wave, while Vp is shown in solid line
Earthq Sci (2014) 27(1):107–115 109
123
3 Depth phases
The depth phases are reflected at free surface upper
hypocenter, and the paths of depth phase and reference
phase are close to each other except the reflected segment.
Hence, the differential time between two phases is domi-
nated by depth, and it is slightly affected by heterogeneity
along propagation path. Benefiting from radiation pattern
of thrust event, the global seismic network provides high-
quality records of the Changning earthquake. We selected
broadband records at Global Seismographic Network.
After removing instrument response and lowpass filtering
(\1 Hz), we chose three high signal–noise-ratio records at
different azimuths (Fig. 4a). When the focal depth is small,
the pP and sP signals may be contaminated by direct P
wave, and manual picking is difficult. The waveform
modeling method, which best fits observation with syn-
thetic waveforms of different focal depths, is a better
choice. The synthetic waveform was computed with three
steps involving effects of mantle, source, and receiver-side
crust (Kikuchi and Kanamori 1982). The source-side crust
model is the same as the previous one, and the velocity
model in the mantle is that of PREM model. The t* (1.0 for
P wave) was adopted to take into account the effect of
inelastic attenuation. Figure 4b shows the comparison
between the filtered observations and the synthetic wave-
forms of different focal depths. All traces were filtered and
aligned with direct P arrival. The differential time between
P and pP shows a clear growth trend in synthetic wave-
forms, and the preferred depth is around 1–2 km.
We also analyzed depth phases as recorded by the
regional network. The sPL phase is an effective one for
determining focal depth at near distance, and it has been
widely used in several moderate earthquake studies (Luo
et al. 2010; Chong et al. 2010). The dominant frequency of
sPL is lower than direct P wave, and the radial component
is much stronger than the vertical one. Three-component
records of JLI pertain to the removed instrument response,
and velocity records were integrated into displacement.
Both the synthetic and observed waveforms are bandpass
filtered between 0.05 and 1.0 Hz. As Fig. 5a shows, the
sPL signal at the radial component is much stronger than
the one at the vertical component. The synthetic wave-
forms of 2 and 3 km fit the observation better than other
4.5
4.4
4.4
4.54.5
4.5
4.5
4.5
4.5
4.5
300
350
400
450
500
550
Mis
mat
ch
0 2 4 6 8 10Depth (km)
CQ.CQT
2.0583
2.0580
1.2589
8.0085
CQ.ROC
1.0596
1.0596
0.8097
0.8092
0.8099
CQ.WAS
2.1081
0.7595
0.7581
2.0098
GZ.BJT
-1.4089
-1.4090
-1.9598
SC.HWS
0.5583
0.5589
1.7096
1.4586
SC.JYA
1.2585
1.2590
2.8095
SC.LBO
-1.7584
-1.7588
-0.3096
-0.3089
-1.9597
SC.LZH
0.6597
0.6599
0.0598
0.0591
SC.MGU
-0.9589
0.5094
0.5079
-1.0597
Pnl Z Pnl R Surface Z Surface R Surface T
YN.YAJ
-1.2584
-1.2597
0.0098
0.0090
-1.3596
YN.ZAT
-1.1094
0.1591
0.1589
(a)
(b)
Fig. 3 a Waveform misfit versus focal depth, b waveform comparison between synthetic (red) and observed waveforms (black line)
110 Earthq Sci (2014) 27(1):107–115
123
ANTO
COLA
TIXI
0
2
4
6
8
10
z (k
m)
0 4 8 12Time (s)
0 4 8 12Time (s)
0 4 8 12Time (s)
(a)
(b)
ANTO COLA TIXI
pP pP pP
Fig. 4 a Teleseismic stations map, b waveform comparison between the teleseismic synthetic (red) and the observed (black) ones
Earthq Sci (2014) 27(1):107–115 111
123
ones. The sPL is also clear for records of Ms4.2 aftershock,
and the differential time between sPL and P suggests that
depth of this aftershock is close to that of the mainshock
(Fig. 5b).
4 Short-period surface wave
At regional networks, we observed strong short-period
surface wave that is an index of shallow earthquake. Tsai
and Aki (1970) proposed that spectrum of surface wave
could be used to constrain focal depth with the well-con-
strained fault plane. The short-period Rg wave also is
considered as an important characteristic of shallow event
(Kafka, 1990; Luo et al. 2011). Both the 90-degree phase
differences between radial and vertical components and
dispersion are helpful to us to identify Rg wave. Figure 6
shows clear Rg wave signals at HWS and LZH stations. In
general, the Rg wave could be observed when epicentral
distance exceeds by about five times of focal depth (Luo
et al. 2011). Consequently, the Rg wave at HWS (dis-
tance = 31 km) suggests that the focal depth of the
Changning earthquake may be not larger than 6 km. The
amplitude ratio of the body wave and the surface wave is
also sensitive to the focal depth (Luo et al. 2011). We
compare the different ratios at the synthetic waveform and
observation, as shown in Fig. 6. As Fig. 6 shows, deeper
focal depth results in weaker Rg wave. At HWS, the best
depth is about 2–4 km, while the other one is about 3–5 km
at LZH. Most of the energy of the short-period Rg wave
was trapped in sediment where inelastic attenuation is
much stronger than that at middle crust. While path of the
body wave bends toward the middle crust, inelastic atten-
uation of the body wave slightly increases with the
0
2
4
6
8
10
Z (
km)
0 4 8Time (s)
0
2
4
6
8
10
Z (
km)
0 4 8Time (s)
(a) (b)
sPL sPL
Fig. 5 a sPL waveform fitting at JLI station for Ms4.8 mainshock, b sPL waveform fitting at JLI station for Ms4.2 aftershock. Red the synthetic
vertical component: gray the synthetic radial component; and blue the observed radial component
112 Earthq Sci (2014) 27(1):107–115
123
distance. Therefore, amplitude ratio between Rg and body
wave at farther stations will be smaller than the one mea-
sured at closer station.
5 Discussion and conclusions
As mentioned above, the Changning earthquake is a thrust
event on ESE fault plane, while theestimated focal depth is
between 2 and 4 km. The preferred depth of 3 km was
obtained from CAP inversion, and it is supported by both
depth phases and short-period surface observations. In the
southern Sichuan depression, thicknesses of Paleozoic and
Mesozoic sediments are about 7 km (Song and Luo 1995),
and so the hypocenter is positioned in the Paleozoic
Dengying Formation. The most-deconstructive earthquake
occurs in the crystalline basement, and Horton et al. (2005)
reported a rare case of a Mw4.2 earthquake that occurred in
Paleozoic sediment in Kentucky, U.S.A. The number of
fellable earthquake at Changning has been significantly
increasing since 2006 (Ruan et al. 2008). In October 2007,
Earthquake Administration of Sichuan Province installed
two temporal broadband seismometers to monitor micro-
seismicity. The location result shows that most small
earthquakes are shallower than 3 km, while stronger events
occurred at greater depths, while the centroid of earth-
quakes between October 18, 2007 and November 12, 2007
lies at about 10 km east of the salt mine. The semi-major
axis of the earthquake cluster is close to that of the fault
plane I of this study’s result. The focal mechanism solution
indicates the axis of the compressive principal stress along
NE. This result is similar to the previous result (Ruan et al.
2008), but it is different from the result of the regional
tectonic stress field (Zhu et al. 2007). Mckenzie (1969)
0
2
4
6
8
10
Z (
km)
0 10 20 30Time (s)
0
2
4
6
8
10
Z (
km)
10 20 30 40
Time (s)
(a) (b)
RgS wave RgS wave
Fig. 6 a Observed (black) and synthetic (red) short-period surface waves at HWS, b observed (black) and synthetic (red) short-period surface
waves at LZH
Earthq Sci (2014) 27(1):107–115 113
123
pointed out that the stress axes obtained from a few
earthquakes might deviate from that of the regional tec-
tonic stress. Another potential interpretation is that the
present tectonic stress is different from the one in geo-
logical time. The rupture fault was formed in different
tectonic stresses, and a strong horizontal stress induced the
thrust sliding.
Changning–Weiyuan region is one among the first pilot
shale-gas fields of China. Since hydraulic fracking
increases concern on seismic hazard, the Changning
earthquake provides a case to study the mechanism of
earthquake in sediment that will be helpful to us to
understand induced seismicity. The salt mining is a his-
torical industry in Sichuan basin, and previous studies
proposed that fluid injection during the salt mining induced
microseismicity (e.g., Lu et al. 2009; Long et al. 2010). At
Changning, the salt deposit is about 2,400–2,900 m deep,
and the deepest injection well is about 3,000 m (Ruan et al.
2008). The number of felt earthquake shows similar vari-
ation with the net injected fluid volume (Ruan et al. 2008).
Injected fluid not only induces seismicity around well but
also possibly diffuses to nearby fault and results in the
increase of pore pressure. The induced seismicity in
Arkansas shows that the fluid injection increases the
potential of deconstructive earthquake at blind faults
(Horton 2012) even tens of kilometers away. Flows in the
lower crust and the upper mantle may enhance stress in the
upper crust, and it leads to the seismogenic fault reaching
critical state (Zoback and Townend 2001). The lower
mantle flow beneath Sichuan basin has been reported in
recent decades, and high-frequency-induced seismicity in
Rongchang region also supported the fact that faults are in
critical state. Therefore, even a small stress perturbation
caused by injected fluid could induce earthquake. Induced
seismicity such as that occurred in the Changning earth-
quake raises public concern on seismic hazard.
Since the Changning earthquake occurred only 5 days
after the April 20, Lushan Ms7.0 earthquake and separation
between two earthquakes is \300 km, the Changning
earthquake raised concern on whether the Lushan earth-
quake would trigger strong earthquake in adjacent region.
There are two main potential mechanisms about earthquake
trigger: static and dynamic triggering mechnisms. Coseis-
mis static displacement changes strain at nearby faults, and
the resulting effect could be described as change of Cou-
lomb failure stress (DCFS). Positive DCFS means that risk
of earthquake increases, and the DCFS threshold of trig-
gering is about 0.1 MPa (King et al. 1994). The coseismic
static displacement decreases with distance as 1/r–1/r2. For
example, in the Mw7.3 Landers earthquake, the DCFS is
only about 0.003 MPa at 200 km far away (Hill et al.
1993). Shan et al. (2013) show that DCFS caused by the
Lushan earthquake at Huayingshan fault is less than
-0.01 MPa. Therefore, the possibility of static trigger is
very low. The amplitude of surface wave excited by large
earthquake decreases with distance, as such displacement
could induce strong stress perturbation. Therefore, the
dynamic triggering is still significant at far field. For
example, the maximum dynamic stress perturbation caused
by the Mw7.9 Denali earthquake is up to 0.12 MPa at
3,000 km far away (Pankow et al. 2004). Most dynamic
triggered events occurred in a few minutes after arrival of
surface wave. However, Brodsky and Prejean (2005) pro-
posed the fluid migration is a potential mechanism of
dynamic trigger, and delay time would be affected by
permeability and diffusion coefficient (Glowacka et al.
2002). The delay time ranges from seconds to days (Mo-
hamad et al. 2000; Hough 2005). After fluid injection in
past decades, rock in sediment may have been saturated
and easier to be triggered. However, there is not clear
creditable clue of triggering.
In summary, focal mechanism of the Changning earth-
quake was obtained from waveform inversion, and the fault
plane I (128�/42�/83�) is possibly the rupture plane. The
focal depth (2–4 km) was determinated with the depth
phases and amplitude ratio of body wave and surface wave.
Such shallow earthquake in Paleozoic sediment is possibly
induced by fluid injection rather than triggered by the
Lushan earthquake.
Acknowledgments The authors thank Dr. Townend and other two
anonymous reviewers for their constructive comments. This work was
supported by China National Special Fund for Earthquake Scientific
Research in Public Interest (201308013), China Postdoctoral Science
Foundation (No. 2012M520431), and the National Natural Science
Foundation of China Grant No. 41204044.
References
Brodsky EE, Prejean SG (2005) New constraints on mechanisms of
remotely triggered seismicity at Long Valley Caldera. J Geophys
Res 110:B04302. doi:10.1029/2004JB003211
Chen W, Ni S, Wang Z, Zeng X, Wei S (2012) Joint inversion with
both local and teleseismic waveforms for source parameters of
the 2010 Kaohsiung earthquake. Chin J Geophys 55(7):
2319–2328 (in Chinese with English abstract)
Chong J, Ni S, Zeng X (2010) sPL, an effective seismic phase for
determining focal depth at near distance. Chin J Geophys 54(11):
2620–2630 (in Chinese with English abstract)
Dawson J, Cummins P, Tregoning P, Leonard M (2008) Shallow
intraplate earthquakes in Western Australia observed by Inter-
ferometric Synthetic Aperture Radar. J Geophys Res 113:
B11408. doi:10.1029/2008JB005807
Eberhart-Phillips D, Oppenheimer DH (1984) Induced seismicity in
The Geysers geothermal area, California. J Geophys Res 89(B2):
1191–1207
Ellsworth WL (2013) Injection-induced earthquakes. Science
341(6142):1225942
Glowacka E, Nava A, de Cossı́o D, Wong V, Farfan F (2002) Fault
slip, seismicity, and deformation in Mexicali Valley, Baja
114 Earthq Sci (2014) 27(1):107–115
123
California, Mexico, after the M7.1 1999 Hector Mine earth-
quake. Bull Seismol Soc Am 92(4):1290–1299
Gupta HK, Sarma SVS, Harinarayana T, Virupakshi G (1996) Fluids
below the hypocentral region of Latur earthquake, India:
geophysical indicators. Geophys Res Lett 23:1569–1572
Healy J, Rubey W, Griggs D, Raleigh C (1968) The Denver
earthquakes. Science 161(3848):1301–1310
Hill DP, Reasenberg PA, Michael AJ, Arabaz WJ, Beroza G,
Brumbaugh D, Brune JN, Castro R, Davis S, dePolo D,
Ellsworth WL, Gomberg J, Harmsen S, House L, Jackson SM,
Johnston MJS, Jones L, Keller R, Malone S, Munguia L, Nava S,
Pechmann JC, Sanford A, Simpson RW, Smith RB, Stark M,
Stickney M, Vidal A, Walter S, Wong V, Zollweg J (1993)
Seismicity remotely triggered by the magnitude 7.3 Landers,
California, earthquake. Science 260:1617–1623
Horton S (2012) Disposal of hydrofracking waste fluid by injection
into subsurface aquifers triggers earthquake swarm in central
Arkansas with potential for damaging earthquake. Seismol Res
Lett 83(2):250–260
Horton S, Kim WY, Withers M (2005) The 6 June 2003 Bardwell,
Kentucky, earthquake sequence: evidence for a locally perturbed
stress field in the Mississippi embayment. Bull Seismol Soc Am
95(2):431–445
Hough SE (2005) Remotely triggered earthquakes following moder-
ate mainshocks (or, why California is not falling into the ocean).
Seismol Res Lett 76(1):58–66
Kafka L (1990) Rg as a depth discriminant for earthquakes and
explosions: a case study in New England. Bull Seismol Soc Am
80(2):373–394
Kaiser A, Holden C, Beavan J, Beetham D, Benitesa R, Celentanob
A, Collettc D, Cousinsa J, Cubrinovskid M, Dellowa G, Denyse
P, Fieldingf E, Frya B, Gerstenbergera M, Langridgea R,
Masseya C, Motaghg M, Pondarda N, McVerrya G, Ristaua J,
Stirlinga M, Thomash J, Umaa SR, Zhao J (2012) The Mw6.2
Christchurch earthquake of February 2011: preliminary report.
N Z J Geol Geophys 55(1):67–90
Keranen K, Savage H, Abers G, Cochran E (2013) Potentially
induced earthquakes in Oklahoma, USA: links between waste-
water injection and the 2011 Mw5.7 earthquake sequence.
Geology. doi:10.1130/G34045.1
Kikuchi M, Kanamori H (1982) Inversion of complex body waves.
Bull Seismol Soc Am 72(2):491–506
King GC, Stein RS, Lin J (1994) Static stress changes and the
triggering of earthquakes. Bull Seismol Soc Am 84(3):935–953
Klose C, Seeber L (2007) Shallow seismicity in stable continental
regions. Seismol Res Lett 78(5):554–562
Long F, Du F, Ruan X, Deng Y, Zhang T (2010) Water injection
triggered earthquakes in the Zigong mineral wells in ETAS
model. Earthq Res China 26(2):164–171 (in Chinese with
English abstract)
Lu G, Peng Y, Gao F (2009) Progress of the study on induced
earthquake and its countermeasure project in Leshan city. Recent
Dev World Seismol 362(2):19–22 (in Chinese with English
abstract)
Luo Y, Ni S, Zeng X, Xie J, Chen Y, Long F (2010) The M5.0
Suining–Tongnan (China) earthquake of 31 January 2010: a
destructive earthquake occurring in sedimentary cover. Chin Sci
Bull 56(6):521–525
Luo Y, Ni S, Zeng X, Zheng Y, Chen Q, Chen Y (2011) A shallow
aftershock sequence in the north-eastern end of the Wenchuan
earthquake aftershock zone. Sci China D Earth Sci. doi:10.1007/
s11430-010-4026-8
McKenzie D (1969) The relation between fault plane solutions for
earthquakes and the directions of the principal stresses. Bull
Seismol Soc Am 59(2):591–601
Mohamad R, Darkal AN, Seber D, Sandvol E, Gomez F, Barazangi M
(2000) Remote earthquake triggering along the Dead Sea Fault in
Syria following the 1995 Gulf of Aqaba earthquake (Ms = 7.3).
Seismol Res Lett 71(1):47–52
Mori J (1991) Estimates of velocity structure and source depth using
multiple P waves from aftershocks of 1987 Elmore Ranch and
Superstition Hills, California, earthquakes. Bull Seismol Soc Am
81:508–523
Ni S, Helmberger D, Pitarka A (2010) Rapid source estimation from
global calibrated paths. Seismol Res Lett 81(3):498–504
Pankow KL, Arabasz WJ, Pechmann JC, Nava SJ (2004) Triggered
seismicity in Utah from the 3 November 2002 Denali fault
earthquake. Bull Seismol Soc Am 94(6B):S332–S347
Ruan X, Cheng W, Zhang Y, Li J, Chen Y (2008) Research of the
earthquakes induced by water injections in salt mines in Chang-
ning, Sichuan. Earthq Res China 24(3):226–234 (in Chinese with
English abstract)
Shan B, Xiong X, Zheng Y, Jin B, Liu C, Xie Z, Hsu H (2013) Stress
changes on major faults caused by 2013 Lushan earthquake, and
its relationship with 2008 Wenchuan earthquake. Sci China
Earth Sci. doi:10.1007/s11430-013-4641-1
Shi Y, Zhu S (2003) Contrast of rheology in the crust and mantle near
Moho reveled by depth variation of earthquake mechanism in
continental China. Chin J Geophys 46(3):359–365 (in Chinese
with English abstract)
Song H, Luo Z (1995) The study of the basement and deep geological
structures of Sichuan basin, China. Earth Sci Front 2(3–4):231–237
Tsai Y, Aki K (1970) Precise focal depth determination from amplitude
spectra of surface waves. J Geophys Res 75(29):5729–5744
Xie J, Ni S, Zeng X (2012) 1D shear wave velocity structure of the
shallow upper crust in central Sichuan Basin. Earthq Res
Sichuan 143(2):20–24 (in Chinese with English abstract)
Zhao L-S, Helmberger D (1994) Source estimation from broadband
regional seismograms. Bull Seismol Soc Am 84(1):91–104
Zheng XF, Ouyang B, Zhang D, Yao Z, Liang J, Zheng J (2009) Technical
system construction of Data Backup Centre for China Seismograph
Network and data support to researches on the Wenchuan earthquake.
Chin J Geophys 52(5):1412–1417 (in Chinese with English abstract)
Zhu L, Helmberger D (1996) Advancement in source estimation
techniques using broadband regional seismograms. Bull Seismol
Soc Am 86(5):1634–1641
Zhu L, Rivera LA (2002) A note on the dynamic and static
displacements from a point source in multilayered media. Geophys
J Int 148(3):619–627
Zhu L, Huang S, Wei H (2007) On fluid-injection induced earthquake
in Rongchang area. J Geod Geodyn 27(6):86–90 (in Chinese
with English abstract)
Zoback M, Townend J (2001) Implications of hydrostatic pore
pressures and high crustal strength for the deformation of
intraplate lithosphere. Tectonophysics 336(1):19–30
Earthq Sci (2014) 27(1):107–115 115
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